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. 2014 Jul 23;7(7):5403–5426. doi: 10.3390/ma7075403

Table 1.

Schematic representation, polarization components, notations, symmetry, space group and basis vectors in the mono-domain phase model. (Adapted with permission from [24], Copyright 2009 Springer)

Polarization components Notation Symmetry Space group Basis vectors
graphic file with name materials-07-05403-i001.jpg P1 = P2 = P3 = 0 paraelectric Tetragonal P4/mm [100], [010], [001]
graphic file with name materials-07-05403-i002.jpg P1 = P2 = 0, P3 ≠ 0 c phase Tetragonal P4mm [100], [010], [001]
graphic file with name materials-07-05403-i003.jpg P1 ≠ 0, P2 = P3 = 0 a phase Orthorhombic P2mm [100], [010], [001]
graphic file with name materials-07-05403-i004.jpg P1 = P2 ≠ 0, P3 = 0 aa phase Orthorhombic C2mm [110], [110], [001]
graphic file with name materials-07-05403-i006.jpg P1 = P2 ≠ 0 < P3 ≠ 0 r phase ( MA) Monoclinic Cm [110], [110], [001]
graphic file with name materials-07-05403-i007.jpg P1 = P2 ≠ 0 > P3 ≠ 0 r phase ( MB) Monoclinic Cm [110], [110], [001]
graphic file with name materials-07-05403-i008.jpg P1 ≠ 0, P2 = 0, P3 ≠ 0 ac phase ( MC) Monoclinic Pm [100], [010], [001]
graphic file with name materials-07-05403-i009.jpg P1 = P2 = P3 ≠ 0 Fo Monoclinic Cm [110], [110], [001]